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Journal of Magnetics 21(3), 374-378 (2016) http://dx.doi.org/10.4283/JMAG.2016.21.3.374 © 2016 Journal of Magnetics A Study on the Transformer Design considering the Inrush Current Reduction in the Arc Welding Machine In-Gun Kim 1 , Huai-Cong Liu 1 , Su-Yeon Cho 2 , and Ju Lee 1 * 1 Department of Electrical Engineering Hanyang University, Seoul 04763, Korea 2 Korea Automotive Technology Institute(KATECH), Cheon-an 31214, Korea (Received 9 March 2016, Received in final form 21 April 2016, Accepted 27 April 2016) The transformer used in an inverter type arc welding machine is designed to use high frequency in order to reduce its size and cost. Also, selecting core materials that fit frequency is important because core loss increases in a high frequency band. An inrush current can occur in the primary coil of transformer during arc welding and this inrush current can cause IGBT, the switching element, to burn out. The transformer design was carried out in A P method and amorphous core was used to reduce the size of transformer. In addition, sheet coil was used for primary winding and secondary winding coil considering the skin effect. This paper designed the transformer core with an air gap to prevent IGBT burnout due to the inrush current during welding and proposed the optimum air gap length. Keywords : arc welding machine, ferrite & amorphous core, inrush current, air gap core 1. Introduction Recent inverter arc welding machine systems can have high speed switching by using high performance switch- ing elements and are controlled in high frequency. Power IC and circuit, transformer, and reactor for switching take up the largest volume among the components of arc welding machine. Therefore, since the capacity of trans- former and reactor is inversely proportional to frequency, it is necessary to operate them in high frequency [1, 2]. Since the capacity of transformer is influenced by magnetic flux density value and the magnetic flux density is determined by core materials, selecting appropriate materials is important. In general, the core materials that are usable in a high frequency band are ferrite, amorph- ous. When they have the same capacity, the differences of two materials are magnetic flux density, production cost, core loss, etc. This paper designed the transformer based on the information mentioned above. 1) The basic design of transformer was carried out using the A P method. 2) The secondary winding coil was formed in a parallel circuit as it has low voltage and high current. 3) PSP coil and sheet coil were used for coil method considering the skin effect and proximity effect. 4) To minimize the size of transformer core, it was made in different materials (ferrite and amorphous) and then compared. Due to the nature of welding machine, when the trans- former core is saturated after the welding rod is in touch with a base metal, then a high current above 1000A flows in the primary winding of transformer. This current is called inrush current and the power IC can be burned out due to the inrush current. Thus, it is important to choose the core size of transformer considering the inrush current during design. The methods to prevent inrush current are as follows. 1) Make the size of core big so that the transformer is not saturated. 2) Maintain the size of transformer core as it is and increase the number of the turns of coil instead. This paper uses an air gap to prevent the saturation of core while maintaining the size and number of turns of core [3, 4]. 2. Transformer Design Method for Welding Machine 2.1. Area Product Design A P design method is one of the methods of transformer ©The Korean Magnetics Society. All rights reserved. *Corresponding author: Tel: +82-2-2220-0342 Fax: +82-2-2295-7111, e-mail: [email protected] ISSN (Print) 1226-1750 ISSN (Online) 2233-6656

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  • Journal of Magnetics 21(3), 374-378 (2016) http://dx.doi.org/10.4283/JMAG.2016.21.3.374

    © 2016 Journal of Magnetics

    A Study on the Transformer Design considering the Inrush Current Reduction

    in the Arc Welding Machine

    In-Gun Kim1, Huai-Cong Liu1, Su-Yeon Cho2, and Ju Lee1*

    1Department of Electrical Engineering Hanyang University, Seoul 04763, Korea2Korea Automotive Technology Institute(KATECH), Cheon-an 31214, Korea

    (Received 9 March 2016, Received in final form 21 April 2016, Accepted 27 April 2016)

    The transformer used in an inverter type arc welding machine is designed to use high frequency in order to

    reduce its size and cost. Also, selecting core materials that fit frequency is important because core loss increases

    in a high frequency band. An inrush current can occur in the primary coil of transformer during arc welding

    and this inrush current can cause IGBT, the switching element, to burn out. The transformer design was

    carried out in AP method and amorphous core was used to reduce the size of transformer. In addition, sheet coil

    was used for primary winding and secondary winding coil considering the skin effect. This paper designed the

    transformer core with an air gap to prevent IGBT burnout due to the inrush current during welding and

    proposed the optimum air gap length.

    Keywords : arc welding machine, ferrite & amorphous core, inrush current, air gap core

    1. Introduction

    Recent inverter arc welding machine systems can have

    high speed switching by using high performance switch-

    ing elements and are controlled in high frequency. Power

    IC and circuit, transformer, and reactor for switching take

    up the largest volume among the components of arc

    welding machine. Therefore, since the capacity of trans-

    former and reactor is inversely proportional to frequency,

    it is necessary to operate them in high frequency [1, 2].

    Since the capacity of transformer is influenced by

    magnetic flux density value and the magnetic flux density

    is determined by core materials, selecting appropriate

    materials is important. In general, the core materials that

    are usable in a high frequency band are ferrite, amorph-

    ous. When they have the same capacity, the differences of

    two materials are magnetic flux density, production cost,

    core loss, etc. This paper designed the transformer based

    on the information mentioned above.

    1) The basic design of transformer was carried out

    using the AP method.

    2) The secondary winding coil was formed in a parallel

    circuit as it has low voltage and high current.

    3) PSP coil and sheet coil were used for coil method

    considering the skin effect and proximity effect.

    4) To minimize the size of transformer core, it was

    made in different materials (ferrite and amorphous) and

    then compared.

    Due to the nature of welding machine, when the trans-

    former core is saturated after the welding rod is in touch

    with a base metal, then a high current above 1000A flows

    in the primary winding of transformer. This current is

    called inrush current and the power IC can be burned out

    due to the inrush current. Thus, it is important to choose

    the core size of transformer considering the inrush current

    during design. The methods to prevent inrush current are

    as follows.

    1) Make the size of core big so that the transformer is

    not saturated.

    2) Maintain the size of transformer core as it is and

    increase the number of the turns of coil instead.

    This paper uses an air gap to prevent the saturation of

    core while maintaining the size and number of turns of

    core [3, 4].

    2. Transformer Design Method for Welding Machine

    2.1. Area Product Design

    AP design method is one of the methods of transformer

    ©The Korean Magnetics Society. All rights reserved.

    *Corresponding author: Tel: +82-2-2220-0342

    Fax: +82-2-2295-7111, e-mail: [email protected]

    ISSN (Print) 1226-1750ISSN (Online) 2233-6656

  • Journal of Magnetics, Vol. 21, No. 3, September 2016 − 375 −

    design and is expressed by the multiplication of Wa and

    Ac. AP method can be expressed in formula 1, formula 2,

    and Fig. 1. The standard for determining the area of Wadepends on the core shape. AP design method can be

    shown as in Fig. 1 [5-7].

    (1)

    (2)

    The Pt is a total power, Bm is the residual magnetic flux,

    Kf is a waveform coefficient, Ku is a window utilization

    factor, f is the switching frequency, J is a current density.

    The maximum window size of AP method must be made

    considering the space factor of coil, so that there is no

    interference between each other when the coil is winded

    inside the window. AP is proportional to Ac and is

    inversely proportional to f, Bm, and J. That is, the volume

    of transformer core gets smaller when it is designed in

    high frequency and magnetic flux density [8]. Since the

    switching current through the IGBT flows in the

    transformer primary, AP must be designed with about 10%

    margin [9]. Figure 2 shows the inverter arc welding

    machine system.

    2.2. Parallel Circuit

    The winding method using parallel circuit is as in Fig.

    3. X represents the start point of coil and X’ represents

    the end point of coil. In the primary size, AA’ and BB’

    are connected in series. The CD of secondary winding

    coil is coiled in the forward direction and EF is coiled in

    the reverse direction. Also, coil C is connected to F and D

    is connected to E, thereby making a total of 2 parallel

    circuits. C’D’E’F’ are connected together. Since the

    secondary winding coil has low voltage and high current

    (77V, 389A), the current is divided into two through 2

    parallel circuits and thus the current density is halved

    [10].

    2.3. PSP Winding and the Sheet Coil

    PSP winding method and sheet coil are used to reduce

    P a cA W A= ×

    4( 10 ) / ( )P t m f uA P B f J K K= × × × × ×

    Fig. 1. AP Design Method.

    Fig. 2. (Color online) Overview of Inverter Arc Welding Machine System.

    Fig. 3. Winding Method using Parallel Circuit.

  • − 376 − A Study on the Transformer Design considering the Inrush Current Reduction in the Arc Welding Machine…

    − In-Gun Kim et al.

    the influence of proximity effect and skin effect.

    (3)

    μ is a permeability of the coil, σ is a conductivity of the

    coil.

    The skin depth δ of coil from formula 3 is 0.554 mm,

    and a coil much thinner than skin depth must be used

    (Primary coil is 0.2 mm, Secondary coil is 0.5 mm). In

    addition, in the high frequency band by the proximity

    effect, the size and status of current changes greatly

    depending on the location of the two parallel coils of

    secondary winding. Therefore, the parallel coil of secondary

    winding must be interleaved with the primary coil and

    have the same locations. Such placed parallel coil have

    the same magnetic flux and magnetic field distribution

    around it and prevents current unbalance [11]. As a result,

    PSP and SPS coil, not PS or SP coil, must be used. Figure

    4 shows the PSP coil method and Fig. 5 shows the

    specifications of transformer designing.

    The two coil methods in Fig. 6 represents the layer coil

    and sheet coil, and both methods have the same current

    density. The two models operate for an hour and their

    temperature saturation was confirmed. Copperplate coil

    and the coil method of PSP model were used based on the

    result of Fig. 6.

    2.4. Comparison according to Core Materials

    To minimize the optimum of the same allowable fre-

    δ = 1

    πfμσ-----------------

    Fig. 4. PSP Winding Method and Sheet Coil.

    Fig. 5. (Color online) Specifications of Transformer Designing.

    Fig. 6. (Color online) Temperature Saturation Curve in the Layer Coil and Sheet Coil Model.

    Fig. 7. (Color online) Transformer made by using Ferrite and

    Amorphous Core.

  • Journal of Magnetics, Vol. 21, No. 3, September 2016 − 377 −

    quency, magnetic flux density needs to be higher. There-

    fore, the transformer was made with ferrite and amorphous

    core that can be used in a 14.4 kHz section. The specifi-

    cations of each transformer are as in Table 1 and Fig. 7.

    Since the amorphous has a magnetic flux density that is

    three times higher than that of ferrite as in Table 1, it has

    lower weight and number of turns of coil within the same

    frequency. Amorphous is better in terms of performance,

    but it requires more precision in production than ferrite

    because multilayered core is made by molding powder

    due to the nature of amorphous production. The two

    models were applied inside the arc welding machine for

    the experiment and the output was satisfying. The

    experiment environment is as in Fig. 8.

    3. Air Gap Core Method

    A very high current flows inside a welding machine as

    its switch repeats shortening and opening. The output

    current of welding machine is as in Fig. 9. The time must

    be more than 6 ms since shortened to satisfy the rated

    current at 600A during the load.

    The inrush current of transformer primary winding

    occurs when the load is connected to the secondary wind-

    ing of transformer and the switch is on. During the rated

    load of welding machine, welding works normally after 5

    ms. The maximum welding time must be within the

    allowable current of the switching element that the inrush

    current of primary winding can endure. If the maximum

    welding time is exceeded, the switching element is burned

    Table 1. Specifications of the Ferrite and Amorphous Core of

    Transformer.

    Value

    Ferrite

    Core TR

    (PM7)

    Amorphous

    Core TR

    (AMCC-250)

    Core Weight (kg) 3.48 2.23

    Coil Weight (kg) 3.79 2.47

    Turn Ratio 32:4 24:3

    Flux Density (T) 0.11 0.45

    Switch Freq. (kHz) 14.4 14.4

    Core Loss (W) 56.84 57.32

    Coil Loss (W) 20.22 10.11

    Efficiency (%) 97.74 96.96

    Fig. 8. (Color online) Experiment System of Arc Welding

    Machine.

    Fig. 9. (Color online) Output Voltage and Current Waveform

    during Load.

    Fig. 10. (Color online) Comparison of Magnetic Flux Satura-

    tion according to Air Gap.

  • − 378 − A Study on the Transformer Design considering the Inrush Current Reduction in the Arc Welding Machine…

    − In-Gun Kim et al.

    out [12, 13]. An air gap (0-5 mm) was given to increase

    the maximum welding time. The inrush current of primary

    winding is decreased as the induced voltage becomes

    smaller by primary winding, since the inductance in the

    core drops when the air gap increases. However, if the air

    gap exceeds 5 mm, the average magnetic flux density

    (amorphous 0.45T) decreases and cannot satisfy the rated

    output during load. The result of finite element analysis

    on the differences of air gap are as in Fig. 10.

    The highest current that can flow in the used IGBT is

    −600~600A. The characteristics of the inrush current of

    primary winding are as in Fig. 11. This waveform shows

    welding after the welding time was set up to 20 ms and

    switch open was made.

    When the time gets above 12.5 ms, the allowable current

    of IGBT is exceeded regardless of air gap. Thus, the

    maximum welding time cannot go beyond 12.5 ms in the

    used IGBT. The model without an air gap exceeds −600A

    at 10 ms of welding time, while a model with 5 mm-air

    gap does not exceed −600A at 10 ms of welding time.

    This enables welding at up to 10 ms. During welding, the

    output at load as well as the allowable current of IGBT

    and maximum welding time must be considered.

    4. Conclusion

    Since an inverter arc welding machine uses high fre-

    quency band, it has an advantage of reducing the size of

    transformer. It is necessary to reduce the size of trans-

    former core to save cost. However, when the size of core

    is decreased, magnetic flux is saturated and huge inrush

    current occurs by the primary winding of transformer.

    The huge inrush current of primary winding can make

    IGBT, the switching element, burn out. As a result, since

    the maximum welding time is proportional to the time of

    the safe operation of IGBT, the transformer was designed

    by inserting an airgap to decrease the inrush current of

    primary welding. It is necessary to appropriately choose

    the maximum length of air gap as it influences the output

    of load.

    Acknowledgment

    This work was supported by the Human Resources

    Program in Energy Technology of the Korea Institute of

    Energy Technology Evaluation and Planning (KETEP),

    granted financial resource from the Ministry of Trade, Industry

    & Energy, Republic of Korea (No. 20154030200900).

    This work was supported by the National Research

    Foundation of Korea (NRF) grant funded by the Korea

    government (Ministry of Science, ICT & Future Planning)

    (No. NRF-2016R1A2A1A05005392).

    References

    [1] L. Zhao, C. F. Foo, and K. J. Tseng, IEEE Trans. Magn.

    35, 3550 (1999).

    [2] Z. Yu, J. L. Liu, X. B. Cheng, and H. Zhang, IEEE Trans.

    Plasma Science 38, 1019 (2010).

    [3] N. H. Kutkut and D. M. Divan, IEEE Trans. Power Elec-

    tronics 13, 202 (1998).

    [4] P. Poulichet, F. Costa, and E. Laboure, IEEE Trans.

    Magn. 39, 998 (2003).

    [5] Colonel Wm T. McLyman, Transformer and Inductor

    Design Handbook, CRC Press, 4th ed. (2011).

    [6] J. D. Lavers and V. Bolborici, IEEE Trans. Magn. 35,

    3541 (1999).

    [7] I. G. Kim, S. Y. Cho, H. J. Park, C. Y. Park, S. H. Ham,

    and J. Lee, Proceeding of the 43th KIEE Annual Summer

    Conference, 450 (2012).

    [8] C. Leung, S. Baek, S. Dutta, and S. Bhattacharya, Energy

    Conversion Congress and Exposition, 1551 (2010).

    [9] R. Prochazka, J. Hlavacek, and K. Draxler, IEEE Trans.

    Magn. 51, Article 2800204 (2015).

    [10] N. Y. Abed and O. A. Mohammed, IEEE Trans. Magn.

    46, 3249 (2010).

    [11] J. Cobos and R. Prieto, IEEE PELS Newsletter 4, 10

    (2004).

    [12] J. Faiz and S. Saffari, IEEE Trans. Magn. 46, 578 (2010).

    [13] A. Bartel, T. Hulsmann, J. Kuhn, and R. Pulch, IEEE

    Trans. Magn. 50, Article 7011904 (2014).

    Fig. 11. (Color online) Comparison of the Waveform of Pri-

    mary Winding Inrush Current according to Air Gap.